1. From microscopic interactions to the dynamics of the fireball in collaboration with: I.Bouras, A. El, O. Fochler, M. Greif, F. Reining, F. Senzel, J. Uphoff, C. Wesp and Zhe Xu - Boltzmann parton transport including radiation - observables at RHIC and LHC (elliptic flow, jets, heavy quarks) - testing and improving the interaction and transport coefficients C. Greiner, INPC 2013, Firenze, 6th june 2013

2. No model can describe all (most) aspects of the medium evolution. QCD thermalization using parton cascade

3. BAMPS: B oltzmann A pproach of M ulti P arton S catterings A transport algorithm solving the Boltzmann-Equations for on-shell partons with pQCD interactions (Z)MPC, VNI/BMS, AMPT Xiong, Shuryak, PRC 49, 2203 (1994) Dumitru, Gyulassy, PLB 494, 215 (2000) Serreau, Schiff, JHEP 0111, 039 (2001) Baier, Mueller, Schiff, Son, PLB 502, 51 (2001) BAMPS: Z. Xu and C. Greiner, PRC 71, 064901 (2005); Z. Xu and C. Greiner, PRC 76, 024911 (2007) collision probability:

4. J.F.Gunion, G.F.Bertsch, PRD 25, 746(1982) T.S.Biro at el., PRC 48, 1275 (1993) S.M.Wong, NPA 607, 442 (1996) screened partonic interactions in leading order pQCD screening mass: LPM suppression : the formation time  g : mean free path radiative part elastic part suppressed!

5. 3-2 + 2-3: thermalization! Hydrodynamic behavior! 2-2: NO thermalization simulation pQCD 2-2 + 2-3 + 3-2 simulation pQCD, only 2-2 at collision center: x T <1.5 fm,  z < 0.4 t fm of a central Au+Au at s 1/2 =200 GeV Initial conditions: minijets p T >1.4 GeV; coupling  s =0.3 p T spectra

6. C. Wesp numerical extraction of viscosity Green-Kubo relation: Christian Wesp et al, Phys. Rev. C 84(2011) F. Reining Felix Reining et al, Phys. Rev. E 85 (2012)

7. Elliptic Flow and Shear Viscosity in 2-3 at RHIC 2-3 Parton cascade BAMPS Z. Xu, CG, H. Stöcker, PRL 101:082302,2008 viscous hydro. Romatschke, PRL 99, 172301,2007  /s at RHIC: 0.08-0.2 x y z

8. R AA ~ 0.052 cf. S. Wicks et al. Nucl.Phys.A784, 426 nuclear modification factor central (b=0 fm) Au-Au at 200 AGeV O. Fochler et al Quenching of jets first realistic 3d results with BAMPS PRL102:202301:2009

10. O. Fochler et al, J. Phys. G 38 (2011)

11. O. Fochler et al, Phys. Rev. C 82 (2010)

12. O. Fochler et al, J. Phys. G 38 (2011)

13. charming probes D c c _ D _ Pre-equil. phase Jan Uphoff, Fochler, Xu, CG, Phys. Rev. C 82 (2010) Heavy Flavor Hadronic phase QGP D D D D J/ ψ e c c c Initial hard parton scatterings Energy loss J/ ψ regeneration J/ ψ dissociation D D c Charm production c _ c _ c _ c _ B B e b _ b Uphoff, Fochler, Xu, CG Phys. Rev. C84 (2011) Uphoff, Fochler, Xu,CG, Phys. Lett. B 717 (2012)

14. Heavy quark scattering Leading order perturbative QCD: t channel is divergent for small t can be fixed to A. Peshier, arXiv:0801.0595 [hep-ph] P.B. Gossiaux, J. Aichelin, Phys.Rev.C78 (2008) by comparing dE/dx to HTL result beyond logarithmic accuracy Introduce a running coupling constant for all channels

15. Heavy quark v 2 and R AA at RHIC PHENIX data, Phys.Rev. C84 (2011) Peterson fragmentation Uphoff, Fochler, Xu, CG Phys. Rev. C84 (2011)

16. v 2 predictions for the LHC only elastic heavy quark processes LHC

17. v 2 predictions for the LHC only elastic heavy quark processes LHC

18. Electron v 2 at LHC only elastic heavy quark processes LHC ALICE data, QM12

19. D meson R AA at LHC – 0-7.5% central only elastic heavy quark processes LHC ALICE data, QM12

20. What can we learn? What can we learn from the models?  No big surprises in going from RHIC to LHC  Too early to rule models out (beside AdS/CFT)  Describing v 2 and R AA simultaneously is challenging good v 2 description: Rad.+ improved el. pQCD (Gossiaux et al.), scaled improved el. pQCD (Uphoff et al.), … good R AA description: Rad.+el. pQCD (Vitev, WHDG, ASW, Cao, …), resonance scattering (Hees et al.) …

21. A Closer Look on the Gunion-Bertsch Approximation

22. The Problems with Gunion-Bertsch

24. color glass condensate see eg Kovchegov, Rischke, Phys.Rev. C56 (1997)

25. Radiative pQCD processes Exact matrix element Kunszt, Pietarinen, Reya, Phys.Rev. D21 (1980) improved Gunion Bertsch (GB) approximation QQqq Fochler, JU, Xu, Greiner, arXiv:1302.5250

26. R AA with improved Gunion-Bertsch Fochler, JU, Xu, Greiner, arXiv:1302.5250 Improved Gunion-Bertsch matrix element

27. Inelastic/radiative pQCD interactions (23 + 32) explain: fast thermalization large collective flow, also of heavy quarks small shear viscosity of QCD semirealistic jet-quenching, also of heavy quarks Summary Future/ongoing analysis and developments: Gunion-Bertsch approximation needs corrections jet-quenching (Mach Cones, ridge, fluctuations) momentum dijet asymmetry hadronisation and afterburning (UrQMD)

28. Riemann problem at finite viscosity Development of a shock plateau I. Bouras et al, PRL 103:032301 (2009)  /s less than 0.1-0.2 Tleft = 400 MeV Tright = 200 MeV t = 1.0 fm/c

29. VISCOUS Solutions … the death of Mach Cones ? I. Bouras et al, arXiv:1201.5005 (2012)

30. Mach cones at relativistic HIC Central collisions and Smooth initial conditions at RHIC energies E_jet = 20 GeV

31. At fixed angle 180 Random position on the semi circle Mach cones at relativistic HIC

32. LPM-effect transport model: incoherent treatment of gg  ggg processes  parent gluon must not scatter during formation time of emitted gluon discard all possible interference effects (Bethe-Heitler regime) ktkt CM frame p1p1 p2p2 lab frame ktkt  = 1 / k t total boost O. Fochler

33. Impact on observables – R AA and v 2 Simulations of R AA and v 2 at 2.76 ATeV α s = 0.3 Elliptic flow is decreased, jet quenching is decreased Effect on R AA is stronger than on v 2 Determined by complex self-screening of rates and relative contributions of different processes to the observables Room for e.g. running coupling, improvement of results possible